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Two planes in F3F^{3} whose sum is F3F^{3} and whose intersection is a line, computed explicitly

Example

Let FF be a field (Field) and let F3F^{3} be the vector space of functions 3F3 \to F with the pointwise operations (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}), where 3={0,1,2}3 = \{0,1,2\}, so an element is x=(x0,x1,x2)x = (x_0, x_1, x_2) indexed from 00. Let e1F3e_1 \in F^{3} have coordinates (0F,1F,0F)(0_F, 1_F, 0_F) and put

U  :=  {xF3:x2=0F},W  :=  {xF3:x0=0F}.U \;:=\; \{\, x \in F^{3} : x_2 = 0_F \,\}, \qquad W \;:=\; \{\, x \in F^{3} : x_0 = 0_F \,\}.

Then:

  1. UU and WW are linear subspaces of F3F^{3} (Linear subspace of a vector space);
  2. U+W=F3U + W = F^{3} (The sum U+WU + W of two linear subspaces and the sum i<nUi\sum_{i<n} U_i of a finite family), a decomposition of xx being x=(x0,x1,0F)+(0F,0F,x2)x = (x_0, x_1, 0_F) + (0_F, 0_F, x_2);
  3. UW={xF3:x0=0F and x2=0F}=span{e1}U \cap W = \{\, x \in F^{3} : x_0 = 0_F \text{ and } x_2 = 0_F \,\} = \operatorname{span}\{e_1\};
  4. the sum is not direct: it is not the case that F3=UWF^{3} = U \oplus W, because UW{0V}U \cap W \ne \{0_V\}.

UU and WW are called planes and UWU \cap W a line, informally and by analogy only; dimension is not available at this point in the library and nothing below uses it.

Facts & Assumptions

Given: A field FF, the vector space F3F^{3} with pointwise operations, the vector e1e_1, and the sets UU and WW as displayed.

[L1]

F3F^{3} is the vector space of functions 3F3 \to F with (x+y)i=xi+yi(x+y)_i = x_i + y_i and (λx)i=λxi(\lambda x)_i = \lambda x_i, where 3={0,1,2}3 = \{0,1,2\}; its zero vector has all three coordinates 0F0_F; and two elements are equal exactly when all three coordinates agree (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}, Vector space over a field, The natural numbers N\mathbb{N} (von Neumann), On N\mathbb{N} the order is membership: m<n    mnm < n \iff m \in n).

[L2]

One-step test: a nonempty TVT \subseteq V with λu+vT\lambda u + v \in T for all λF\lambda \in F and u,vTu, v \in T is a linear subspace (One-step subspace test: a nonempty WVW \subseteq V is a linear subspace if and only if λu+vW\lambda u + v \in W for all λF\lambda \in F and u,vWu, v \in W, Linear subspace of a vector space).

[L3]

The intersection of a nonempty family of linear subspaces is a linear subspace (The intersection of a nonempty family of linear subspaces of VV is a linear subspace of VV).

[L4]

U+W={u+w:uU, wW}U + W = \{\, u + w : u \in U,\ w \in W \,\}, and it is a linear subspace (The sum U+WU + W of two linear subspaces and the sum i<nUi\sum_{i<n} U_i of a finite family).

[L6]

For two summands, F3=UWF^{3} = U \oplus W requires U+W=F3U + W = F^{3} and UW={0V}U \cap W = \{0_V\} (Internal direct sum V=i<nUiV = \bigoplus_{i<n} U_i: the sum is everything and each summand meets the sum of the others only in 0V0_V).

[L7]

In a field: 1F0F1_F \ne 0_F; λ1F=λ\lambda 1_F = \lambda; 0Fλ=0F0_F \lambda = 0_F (Multiplication by zero: 0a=00 \cdot a = 0) and multiplication is commutative, so λ0F=0F\lambda 0_F = 0_F; and 0F0_F is the additive identity (Field).

Verification

technique · direct
1.1

F3F^{3} is the set of functions 3F3 \to F with coordinatewise operations, and e1e_1 has coordinates (0F,1F,0F)(0_F, 1_F, 0_F), so e1F3e_1 \in F^{3}.

L1L7
1.2

UU is a linear subspace: it contains the zero vector, whose coordinate at index 22 is 0F0_F, so it is nonempty; and for λF\lambda \in F and u,vUu, v \in U the vector λu+v\lambda u + v has (λu+v)2=λu2+v2=λ0F+0F=0F(\lambda u + v)_2 = \lambda u_2 + v_2 = \lambda 0_F + 0_F = 0_F, so it lies in UU. The same argument at index 00 shows WW is a linear subspace.

L1L2L7
1.3

UW={xF3:x0=0F and x2=0F}U \cap W = \{\, x \in F^{3} : x_0 = 0_F \text{ and } x_2 = 0_F \,\}, directly from the two defining conditions.

L1
1.4

The scalar multiples of e1e_1 are exactly the vectors with coordinates (0F,λ,0F)(0_F, \lambda, 0_F): (λe1)0=λ0F=0F(\lambda e_1)_0 = \lambda 0_F = 0_F, (λe1)1=λ1F=λ(\lambda e_1)_1 = \lambda 1_F = \lambda and (λe1)2=λ0F=0F(\lambda e_1)_2 = \lambda 0_F = 0_F. Conversely a vector xx with x0=x2=0Fx_0 = x_2 = 0_F agrees with x1e1x_1 e_1 at all three indices, so x=x1e1x = x_1 e_1.

L1L7
2.1

Claim 1 is step 1.2.

step 1.2L2
2.2

Claim 3: by steps 1.3 and 1.4 the intersection UWU \cap W is exactly {λe1:λF}\{\, \lambda e_1 : \lambda \in F \,\}, which is span{e1}\operatorname{span}\{e_1\}; it is a linear subspace, being an intersection of two of them.

step 1.3step 1.4L3L5
2.3

Claim 2: given xF3x \in F^{3}, put u:=(x0,x1,0F)u := (x_0, x_1, 0_F) and w:=(0F,0F,x2)w := (0_F, 0_F, x_2). Then uUu \in U and wWw \in W by step 1.2, and u+wu + w has coordinates (x0+0F,  x1+0F,  0F+x2)=(x0,x1,x2)(x_0 + 0_F,\; x_1 + 0_F,\; 0_F + x_2) = (x_0, x_1, x_2), so u+w=xu + w = x. Hence F3U+WF^{3} \subseteq U + W, and the reverse inclusion holds because U+WU + W is a subset of F3F^{3}.

step 1.2L1L4L7
3.1

Claim 4: e1UWe_1 \in U \cap W by step 2.2, and e10Ve_1 \ne 0_V because its coordinate at index 11 is 1F0F1_F \ne 0_F; so UW{0V}U \cap W \ne \{0_V\} and the condition for a direct sum of two summands fails.

step 2.2L1L6L7
4.1

Claims 1, 2, 3 and 4 are steps 2.1, 2.3, 2.2 and 3.1: the two planes have sum F3F^{3} and intersection span{e1}\operatorname{span}\{e_1\}, and the sum is not direct.

step 2.1step 2.2step 2.3step 3.1

Remarks

  • A sum can be everything without being direct. Condition (D1) holds here and (D2) fails, and the two are independent: the failure is exactly the nonzero overlap span{e1}\operatorname{span}\{e_1\}. Concretely, e1e_1 decomposes in more than one way, for instance as e1+0Ve_1 + 0_V with e1Ue_1 \in U and as 0V+e10_V + e_1 with e1We_1 \in W.

  • The intersection did not have to be computed by hand to know it is a subspace, since intersections of linear subspaces always are (The intersection of a nonempty family of linear subspaces of VV is a linear subspace of VV). What the computation adds is the identification of that subspace as span{e1}\operatorname{span}\{e_1\}, which is the point of the example.

  • Everything here is over an arbitrary field. No order, no square roots and no counting are used; the only field facts needed are 1F0F1_F \ne 0_F and the identity laws.

Depends on

Used by

Nothing in the library uses this result yet.

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Sources